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Modelling of non-thermal radiation from pulsar wind nebulae

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Presentation on theme: "Modelling of non-thermal radiation from pulsar wind nebulae"— Presentation transcript:

1 Modelling of non-thermal radiation from pulsar wind nebulae
Joshua L. Botha B.Sc. Hons.

2 Outline Short introduction on non-thermal radiation mechanisms of pulsar wind nebulae Workings of mathematical model used Results of model application on one known source and one unknown source Conclusions drawn from model

3 Synchrotron radiation
The angle between the direction of the magnetic field and the direction of the total velocity of a particle is called a pitch angle The Lorentz force acts upon any charged particle moving in a magnetic field The charged particle rotates around magnetic field line The centripetal acceleration leads to the emission of photons Typically in an astrophysical system the particle spectrum can be described by a power law

4 Synchrotron radiation
Assuming the pitch angle distribution is isotropic the synchrotron radiation is calculated by integrating over pitch angle as well as electron energy, leading to the following equation:

5 Inverse Compton radiation
Energetic particles can collide with photons Collision causes the particle to lose energy, but the photon energy increases greatly Sources of photons can be CMBR, IR photons, starlight, and sychrotron emissions

6 Pulsar wind nebulae Pulsars are stellar remnants of supernova explosions Due to the conservation of angular momentum of the parent star the produced pulsar has a high rotation energy Rotation rate decreases over time, therefore the rotational energy must be converted into other forms The two main energy conversions are magnetic dipole radiation and injection of relativistic electrons/positrons (supersonic pulsar wind) into surrounding medium

7 Pulsar wind nebulae Due to the conservation of magnetic flux the pulsars magnetic field is frozen into and carried out by the pulsar wind At a certain point the pressure of the injected pulsar wind is the same as the pressure of the surroundings, causing a termination shock after which the particles move at sub sonic speeds The injected particles interact with the surrounding medium causing synchrotron and inverse Compton radiation

8 Model

9 results Some observed parameters Some parameters used B0 = 1.3x102 μG
Lcurrent = 3.3x1037 erg/s Distance = 4.6 kpc Tage = 4.8 kyrs ηR = 0.3 ηX = 0.06 r1 = 1.4 pc r2 = 0.2 pc The model predicted a current magnetic field strength of 250 μG, where the observed strength is 300 μG.

10 results Known: further than 6 kpc.
Parameters used: distance = 6 kpc, Tage = 15 kyrs, L0 = 1.5x1039 erg/s, ηR = 0.2, ηX = 0.05, τ = 6 kyrs. Predicted B = 0.3 μG.

11 conclusion The model can be used to obtain first-order estimate
A dual electron energy population is not necessarily a result of the long term pulsar evolution (as often stated) The predicted magnetic field strength for an old PWN is less than the cosmic background magnetic field strength ηR seems to be a factor 10 larger than ηX.


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